WO2005109970A1 - Procede permettant d'obtenir des etats stables pour un plasma dense a haute temperature - Google Patents
Procede permettant d'obtenir des etats stables pour un plasma dense a haute temperature Download PDFInfo
- Publication number
- WO2005109970A1 WO2005109970A1 PCT/RU2005/000284 RU2005000284W WO2005109970A1 WO 2005109970 A1 WO2005109970 A1 WO 2005109970A1 RU 2005000284 W RU2005000284 W RU 2005000284W WO 2005109970 A1 WO2005109970 A1 WO 2005109970A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- plasma
- gravitational
- emission
- energy
- states
- Prior art date
Links
- 238000000034 method Methods 0.000 title claims abstract description 25
- 238000001228 spectrum Methods 0.000 claims abstract description 29
- 230000005291 magnetic effect Effects 0.000 claims abstract description 28
- 230000007704 transition Effects 0.000 claims abstract description 17
- 230000004927 fusion Effects 0.000 claims abstract description 15
- 230000006835 compression Effects 0.000 claims abstract description 14
- 238000007906 compression Methods 0.000 claims abstract description 14
- 238000010791 quenching Methods 0.000 claims abstract description 12
- 230000000171 quenching effect Effects 0.000 claims abstract description 12
- 230000003321 amplification Effects 0.000 claims abstract description 9
- 238000003199 nucleic acid amplification method Methods 0.000 claims abstract description 9
- 230000002706 hydrostatic effect Effects 0.000 claims abstract description 8
- 238000012546 transfer Methods 0.000 claims abstract description 8
- 239000000203 mixture Substances 0.000 claims abstract description 7
- 230000002269 spontaneous effect Effects 0.000 claims abstract description 7
- 239000007789 gas Substances 0.000 claims description 17
- 229910052739 hydrogen Inorganic materials 0.000 claims description 12
- 239000001257 hydrogen Substances 0.000 claims description 12
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 claims description 9
- 230000015572 biosynthetic process Effects 0.000 claims description 9
- 238000002347 injection Methods 0.000 claims description 9
- 239000007924 injection Substances 0.000 claims description 9
- 238000006243 chemical reaction Methods 0.000 claims description 8
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 claims description 6
- 229910052799 carbon Inorganic materials 0.000 claims description 6
- 239000007809 chemical reaction catalyst Substances 0.000 claims description 2
- 210000002381 plasma Anatomy 0.000 abstract description 111
- 230000005461 Bremsstrahlung Effects 0.000 description 14
- 150000002500 ions Chemical class 0.000 description 10
- 125000004429 atom Chemical group 0.000 description 9
- 239000002245 particle Substances 0.000 description 9
- 239000000243 solution Substances 0.000 description 9
- 238000005755 formation reaction Methods 0.000 description 8
- 230000006870 function Effects 0.000 description 8
- 230000005484 gravity Effects 0.000 description 8
- 230000005255 beta decay Effects 0.000 description 5
- 238000011161 development Methods 0.000 description 5
- 230000003993 interaction Effects 0.000 description 5
- 238000010584 magnetic trap Methods 0.000 description 5
- 230000008569 process Effects 0.000 description 5
- 230000005284 excitation Effects 0.000 description 4
- YZCKVEUIGOORGS-OUBTZVSYSA-N Deuterium Chemical compound [2H] YZCKVEUIGOORGS-OUBTZVSYSA-N 0.000 description 3
- 238000013461 design Methods 0.000 description 3
- 229910052805 deuterium Inorganic materials 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 238000000295 emission spectrum Methods 0.000 description 3
- 238000002474 experimental method Methods 0.000 description 3
- 150000002431 hydrogen Chemical class 0.000 description 3
- 229910052743 krypton Inorganic materials 0.000 description 3
- DNNSSWSSYDEUBZ-UHFFFAOYSA-N krypton atom Chemical compound [Kr] DNNSSWSSYDEUBZ-UHFFFAOYSA-N 0.000 description 3
- 230000004807 localization Effects 0.000 description 3
- 238000005086 pumping Methods 0.000 description 3
- 238000006467 substitution reaction Methods 0.000 description 3
- 230000009466 transformation Effects 0.000 description 3
- 229910052724 xenon Inorganic materials 0.000 description 3
- FHNFHKCVQCLJFQ-UHFFFAOYSA-N xenon atom Chemical compound [Xe] FHNFHKCVQCLJFQ-UHFFFAOYSA-N 0.000 description 3
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 2
- 238000013459 approach Methods 0.000 description 2
- 238000004364 calculation method Methods 0.000 description 2
- 238000010168 coupling process Methods 0.000 description 2
- 238000005859 coupling reaction Methods 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 230000005281 excited state Effects 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 230000010354 integration Effects 0.000 description 2
- 230000007246 mechanism Effects 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 230000005610 quantum mechanics Effects 0.000 description 2
- 230000005855 radiation Effects 0.000 description 2
- 229910052717 sulfur Inorganic materials 0.000 description 2
- 229910052722 tritium Inorganic materials 0.000 description 2
- 230000005428 wave function Effects 0.000 description 2
- 230000009471 action Effects 0.000 description 1
- 230000002730 additional effect Effects 0.000 description 1
- 239000000654 additive Substances 0.000 description 1
- 230000000996 additive effect Effects 0.000 description 1
- 238000004458 analytical method Methods 0.000 description 1
- 229910052786 argon Inorganic materials 0.000 description 1
- 239000003990 capacitor Substances 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 239000003054 catalyst Substances 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 230000001143 conditioned effect Effects 0.000 description 1
- 238000012790 confirmation Methods 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000006731 degradation reaction Methods 0.000 description 1
- 230000005520 electrodynamics Effects 0.000 description 1
- 238000010894 electron beam technology Methods 0.000 description 1
- 238000004471 energy level splitting Methods 0.000 description 1
- 230000002349 favourable effect Effects 0.000 description 1
- 238000005290 field theory Methods 0.000 description 1
- 239000012530 fluid Substances 0.000 description 1
- 238000005288 gauge theory Methods 0.000 description 1
- 230000001939 inductive effect Effects 0.000 description 1
- 230000014759 maintenance of location Effects 0.000 description 1
- 238000013178 mathematical model Methods 0.000 description 1
- 230000003340 mental effect Effects 0.000 description 1
- 229910052754 neon Inorganic materials 0.000 description 1
- GKAOGPIIYCISHV-UHFFFAOYSA-N neon atom Chemical compound [Ne] GKAOGPIIYCISHV-UHFFFAOYSA-N 0.000 description 1
- 229910052756 noble gas Inorganic materials 0.000 description 1
- 150000002835 noble gases Chemical class 0.000 description 1
- 238000010606 normalization Methods 0.000 description 1
- 230000036470 plasma concentration Effects 0.000 description 1
- 230000000717 retained effect Effects 0.000 description 1
- 230000002311 subsequent effect Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21B—FUSION REACTORS
- G21B1/00—Thermonuclear fusion reactors
- G21B1/05—Thermonuclear fusion reactors with magnetic or electric plasma confinement
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- H05H1/00—Generating plasma; Handling plasma
- H05H1/02—Arrangements for confining plasma by electric or magnetic fields; Arrangements for heating plasma
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- H05H1/00—Generating plasma; Handling plasma
- H05H1/02—Arrangements for confining plasma by electric or magnetic fields; Arrangements for heating plasma
- H05H1/16—Arrangements for confining plasma by electric or magnetic fields; Arrangements for heating plasma using externally-applied electric and magnetic fields
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- H05H1/00—Generating plasma; Handling plasma
- H05H1/02—Arrangements for confining plasma by electric or magnetic fields; Arrangements for heating plasma
- H05H1/22—Arrangements for confining plasma by electric or magnetic fields; Arrangements for heating plasma for injection heating
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E30/00—Energy generation of nuclear origin
- Y02E30/10—Nuclear fusion reactors
Definitions
- the present invention relates to a method of forming stable states of a dense high- temperature plasma which can be used, for example, for controlled fusion.
- the existing state of the art related to the realization of stable states of a dense high- temperature plasma applicable for the purposes of nuclear fusion can be defined as a stage of the formation and confinement of a plasma by a magnetic field in devices which make it possible to realize separate techniques of the claimed method but not the method as such, i.e., a method of achieving a stable state of a dense high-temperature plasma.
- the claimed method has no close analogs.
- a heavy-current pulsed discharge which is shaped with the aid of a cylindrical discharge chamber (whose end faces function as electrodes) which is filled with a working gas (deuterium, hydrogen, a deuterium-tritium mixture at a pressure of 0.5 tolO mm Hg, or noble gases at a pressure of 0.01 toO.l mm Hg).
- a working gas deuterium, hydrogen, a deuterium-tritium mixture at a pressure of 0.5 tolO mm Hg, or noble gases at a pressure of 0.01 toO.l mm Hg.
- Magnetic traps are devices which are capable of confining a high-temperature plasma for a sufficiently long time within a limited volume and which are described in Artsimovich L.A., "Closed Plasma Configurations", Moscow, Atomizdat, 1969.
- To magnetic traps of closed type on which hopes to realize the conditions of controlled nuclear fusion (CNU) were pinned for a long time
- Tokamak, Spheromak and Stellarator type in various modifications (Lukyanov S.Yu., "Hot Plasma and CNU", Moscow, Atomizdat, 1975 (in Russian)).
- a ring current creating a rotary transformation of mag- netic lines of force is excited in the very plasma.
- Spheromak represents a compact torus with a toroidal magnetic field inside a plasma.
- Rotary transformation of magnetic lines of force, effected without exciting a toroidal current in plasma, is realized in Stellarators (Volkov E.D. et al., "Stellarator", Moscow, Nauka, 1983 (in Russian)).
- Open-type magnetic traps with a linear geometry are: a magnetic bottle, an ambipolar trap, a gas-dynamic type trap (Ryutov D.D., "Open traps", Uspekhi Fizicheskikh Nauk, 1988, vol. 154, p. 565).
- the present invention relates to a method of forming stable states of a dense high-temperature plasma, which comprises the following steps: a) generation of a dense high-temperature plasma from hydrogen and isotopes thereof with the aid of pulsed heavy-current discharges; b) injection of the plasma from the area of a magnetic field with parameters corresponding to the conditions of gravitational emission of electrons with a banded energy spectrum; c) energy transfer along the spectrum.
- the energy transfer (step c) is performed by cascade transition into the long wavelength region of eV-energy to the state of locking and amplification of the gravitational emission and simultaneous compression to the states of hydrostatic equilibrium, and in the formation of said states in the composition of a working gas multielectron atoms are used for quenching the spontaneous gravitational emission from the ground energy levels of the keV-region electron in the proper gravitational field. It is preferable that in one of the embodiment of the invention for obtaining stable states of a dense high-temperature plasma use is made of hydrogen and multielectron atoms, such as krypton, xenon, and other allied elements (neon, argon).
- the claimed method provides a scheme for forming stable states of a dense high- temperature plasma, which scheme comprises a device for supplying a working gas, a discharge chamber, a discharge circuit, a chamber for forming a stable plasma bunch. If and when necessary, each of the cited blocks of the scheme can be fitted with appropriate measuring equipment.
- the invention is illustrated by a circuit diagram of a pulsed heavy-current magnetic- compression discharge on multiply charged ions with conical coaxial electrodes, in which : 1. a fast-acting valve for supplying a working gas into a gap between an internal electrode
- an external electrode (3) (2) and an external electrode (3); 2. an external electrode; 3. an internal electrode has a narrowing surface close to conical one; 4. a diverter channel which prevents the entrance of admixtures into the compression area; 5. a discharge circuit; 6. an area of compression by a magnetic field; 7. an area of compression due to efflux current in the outgoing plasma jet and subsequent compression by the emitted gravitational field.
- stable states of a dense high-temperature plasma denotes the states of hydrostatic equilibrium of a plasma, when the gas-dynamic pressure is counterbalanced by the pressure of a magnetic field or, in the present case, by the pressure of the emitted gravitational field.
- plasma parameters corresponding to gravitational emission of electrons denotes parameters which are in the above-indicated range of pressures and temperatures.
- locking of avitational emission in plasma denotes the state of gravitational emission in a plasma ,which takes place when its emission frequency and electron Lang- muir frequency are equal.
- locking of the emission takes place for two reasons: - energy transfer along the spectrum into the long wavelength region as a result of cas- cade transitions into the long wavelength region with attaining emission frequency (10 — 10 ) with plasma Langmuir frequency equal to the electron one, this being the condition of locking gravitational emission in plasma; - quenching spontaneous gravitational emission of electrons from the ground energy levels by multielectron atoms, when the energy of an excited electron is transferred to an ion with corresponding energy levels, leading to its ionization.
- amplification of gravitational emission denotes amplification which takes place when the gravitational emission is locked, because, with the locking conditions having been fulfilled, the gravitational emission remains in plasma with sequential emission of the total energy of the gravitational field locked in the plasma.
- Equations (1) through (5) describe the equilibrium states of particles (stationary states) in the proper gravitational field and define the localization region of the field characterized by the constant K that satisfies the equilibrium state. These stationary states are sources of the field with the constant G, and condition (3) provides matching the solution with the gravitational constants K and G.
- the proposed model in the physical aspect is compatible with the principles of quantum mechanics principles, and the gravitational field with the constants K and A at a certain, quite definite distance specified by the equilibrium state transforms into the filed having the constant G and satisfying, in the weak field limit, the Poisson equation.
- the set of equations (1) through (5) is of interest for the problem of stationary states, i.e., the problem of energy spectrum calculations for an elementary source in the own gravitational field. In this sense it is reasonable to use an analogy with electrodynamics, in particular, with the problem of electron stationary states in the Coulomb field. Transition from the Schrodinger equation to the Klein-Gordon relativistic equations allows taking into account the fine structure of the electron energy spectrum in the Coulomb field, whereas transition to the Dirac equation allows taking into account the relativistic fine struc ture and the energy level splitting associated with spin-orbital interaction.
- Equations (6) — ⁇ 8) follow from equations (14) — ( 15) ⁇ v T ⁇ a v -t- W ' 0 (14)
- Condition (9) defines r sweep- whereas equations (10) through (12) are the boundary conditions and the normalization condition for the function /, respectively.
- the presented numerical estimates for the electron show that within the range of its localization, with K ⁇ 10 31 N m 2 kg “2 and ⁇ 10 29 m “2 , there exists the spectrum of stationary states in the proper gravitational field.
- the numerical value of K is, certainly, universal for any elementary source, whereas the value of A is defined by the rest mass of the elementary source.
- the distance at which the gravitational field with the constant K is localized is less than the Compton wavelength, and for the electron, for example, this value is of the order of its classical radius. At distances larger than this one, the gravitational field is characterized by the constant G, i.e., cor- rect transition to Classical GTR holds.
- Beta-asymmetry was observed experimentally only in ⁇ -decay of heavy nuclei in magnetic field (for example, 27 C 60 in the known experiment carried out by Wu (Wu Ts.S., Moshkovskii S.A., Beta-decay, Atomizdat, Moscow, 1970 (in Russian)).
- Wu Wang Ts.S., Moshkovskii S.A., Beta-decay, Atomizdat, Moscow, 1970 (in Russian)
- t H 3 where the ⁇ -decay asymmetry al- ready must not take place, similar experiments were not carried out
- Plasma must comprise two components, with multiply charged ions added to hydrogen, these ions being necessary for quenching spontaneous emission of electrons from the ground energy levels in the own gravitational field
- these ions being necessary for quenching spontaneous emission of electrons from the ground energy levels in the own gravitational field
- Quenching of the lower excited states of the electrons will be particularly effective in the presence of a resonance between the energy of excited electron and the energy of electron excitation in the ion (in the limit, most favorable case — ionization energy)
- a principal solution of the problem is a method of confining of an already heated plasma in an emitted gravitational field in a second step, after the plasma has been compressed, heated and retained during this period by the magnetic field.
- Plasma must be injected from the magnetic field region, but with subsequent pumping of energy from the region of the plasma found in the magnetic field. It is just to these conditions that, among other things, there corresponds the original circuit diagram of a magnetoplasma compressor, presented in the speci- fication to the Application.
- the claimed method is realized in the following manner (see the diagram): through a quick-acting valve 1 a two-component gas (hydrogen + a multielectron gas) is supplied into a gap between coaxial conical electrodes 2, 3, to which voltage is fed through a discharge circuit 5. A discharge creating a magnetic field flows between the electrodes. Under the pressure of the arising amperage, plasma is accelerated along the channel. At the outlet in a region 7 the flow converges to the axis, where a region of compression with high density and temperature originates. The formation of the region of compression 7 is favored by efflux currents which flow in the outgoing plasma jet.
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- General Engineering & Computer Science (AREA)
- High Energy & Nuclear Physics (AREA)
- Plasma Technology (AREA)
Abstract
La présente invention se rapporte à un procédé permettant d'obtenir des états stables pour un plasma dense à haute température, notamment pour des plasmas destinés à une fusion contrôlée. Le procédé selon l'invention consiste: à générer un plasma dense à haute température à l'aide de décharges de haute intensité pulsées; puis à injecter le plasma issu de la zone d'un champ magnétique présentant des paramètres correspondant aux conditions d'émission gravitationnelle d'électrons avec un spectre de puissance en bandes ; et à procéder à un transfert d'énergie le long du spectre (transition en cascade) dans la zone de longueurs d'onde élevées (d'énergie eV), ce qui entraîne le verrouillage et l'amplification de l'émission gravitationnelle dans le plasma ainsi que la compression de ce dernier pour qu'il atteigne un état d'équilibre hydrostatique. Des atomes à électrons multiples constituent un élément obligatoire dans la composition d'un gaz de travail, afin d'affaiblir l'émission gravitationnelle spontanée issue de l'état normal d'énergie (la zone keV) de l'électron dans le champ gravitationnel approprié.
Priority Applications (10)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| AU2005242054A AU2005242054B2 (en) | 2004-11-30 | 2005-05-24 | Method of forming stable states of dense high-temperature plasma |
| JP2007542959A JP2008522362A (ja) | 2004-11-30 | 2005-05-24 | 高密度高温プラズマの安定状態を形成する方法 |
| US10/570,857 US20070058770A1 (en) | 2004-11-30 | 2005-05-24 | Method of forming stable states of sense high-temperature plasma |
| BRPI0506556-9A BRPI0506556A (pt) | 2004-11-30 | 2005-05-24 | método de formação de estados estáveis de plasma denso de alta temperatura |
| EP05749491A EP1673966A4 (fr) | 2004-11-30 | 2005-05-24 | Procede permettant d'obtenir des etats stables pour un plasma dense a haute temperature |
| CA002538368A CA2538368A1 (fr) | 2004-11-30 | 2005-05-24 | Procede permettant d'obtenir des etats stables pour un plasma dense a haute temperature |
| NZ548650A NZ548650A (en) | 2004-11-30 | 2005-05-24 | Method of forming stable states of dense high-temperature plasma in generating fusion energy |
| CN2005800071699A CN1954391B (zh) | 2004-11-30 | 2005-05-24 | 形成稠密高温等离子体的稳定态的方法 |
| US12/270,123 US20090152094A1 (en) | 2004-11-30 | 2008-11-13 | Method of forming stable states of dense high-temperature plasma |
| US14/316,387 US20160027533A1 (en) | 2004-11-30 | 2014-06-26 | Method of forming stable states of dense high-temperature plasma |
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| RU2004135022 | 2004-11-30 | ||
| RU2004135022/06A RU2273968C1 (ru) | 2004-11-30 | 2004-11-30 | Способ формирования устойчивых состояний плотной высокотемпературной плазмы |
Related Child Applications (2)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US10/570,857 A-371-Of-International US20070058770A1 (en) | 2004-11-30 | 2005-05-24 | Method of forming stable states of sense high-temperature plasma |
| US12/270,123 Continuation-In-Part US20090152094A1 (en) | 2004-11-30 | 2008-11-13 | Method of forming stable states of dense high-temperature plasma |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| WO2005109970A1 true WO2005109970A1 (fr) | 2005-11-17 |
Family
ID=35320612
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| PCT/RU2005/000284 WO2005109970A1 (fr) | 2004-11-30 | 2005-05-24 | Procede permettant d'obtenir des etats stables pour un plasma dense a haute temperature |
Country Status (10)
| Country | Link |
|---|---|
| EP (1) | EP1673966A4 (fr) |
| JP (3) | JP2008522362A (fr) |
| KR (1) | KR100877367B1 (fr) |
| CN (1) | CN1954391B (fr) |
| AU (1) | AU2005242054B2 (fr) |
| BR (1) | BRPI0506556A (fr) |
| CA (1) | CA2538368A1 (fr) |
| NZ (1) | NZ548650A (fr) |
| RU (1) | RU2273968C1 (fr) |
| WO (1) | WO2005109970A1 (fr) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2008063254A2 (fr) * | 2006-08-18 | 2008-05-29 | Unified Gravity Corporation | Dispositif de fusion hydrogène-lithium, procédé et applications |
| JP2013016507A (ja) * | 2004-11-30 | 2013-01-24 | Zakrytoe Aktsionernoe Obschestvo Rustermosintez | 高密度高温プラズマの安定状態を形成する方法 |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| RU2007105087A (ru) * | 2007-02-12 | 2008-08-20 | Борис Федорович Полторацкий (RU) | Плазменный преобразователь энергии и электромагнитный вихревой реактор для его осуществления |
| US20150380113A1 (en) | 2014-06-27 | 2015-12-31 | Nonlinear Ion Dynamics Llc | Methods, devices and systems for fusion reactions |
| AU2014302152A1 (en) * | 2013-06-27 | 2016-02-18 | Nonlinear Ion Dynamics, Llc. | Methods, devices and systems for fusion reactions |
| RU2710865C1 (ru) * | 2019-06-19 | 2020-01-14 | Акционерное общество "Концерн воздушно-космической обороны "Алмаз - Антей" | Плазменный источник излучения |
Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4292125A (en) * | 1978-08-21 | 1981-09-29 | Massachusetts Institute Of Technology | System and method for generating steady state confining current for a toroidal plasma fusion reactor |
| SU1216805A1 (ru) * | 1984-03-15 | 1986-03-07 | Предприятие П/Я В-8851 | Способ создани стационарного тока в плазме |
| RU2067360C1 (ru) * | 1994-01-25 | 1996-09-27 | Михаил Агеевич Поломарчук | Способ получения высокотемпературной плазмы |
| RU2096934C1 (ru) * | 1995-11-29 | 1997-11-20 | Милья Аркадьевич Маргулис | Способ получения высокотемпературной плазмы и осуществления термоядерных реакций |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0750179B2 (ja) * | 1984-06-18 | 1995-05-31 | 松永 誠子 | ホログラフイ−の技術を利用して物質にエネルギ−を与える方法、及び、その装置 |
| JPH11238947A (ja) * | 1998-02-18 | 1999-08-31 | Matsunaga Shigeko | 半導体レーザーアレイ可変発振ホログラムによる半導体レーザーアレイ可変発振ホログラムビンを利用した重力波併用ホログラフィー核融合炉ビンと重力波ホログラフィーの方法、及び、その装置。 |
| RU2273968C1 (ru) * | 2004-11-30 | 2006-04-10 | Закрытое акционерное общество "Рустермосинтез" | Способ формирования устойчивых состояний плотной высокотемпературной плазмы |
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2004
- 2004-11-30 RU RU2004135022/06A patent/RU2273968C1/ru not_active IP Right Cessation
-
2005
- 2005-05-24 KR KR1020067015446A patent/KR100877367B1/ko not_active IP Right Cessation
- 2005-05-24 NZ NZ548650A patent/NZ548650A/xx not_active IP Right Cessation
- 2005-05-24 EP EP05749491A patent/EP1673966A4/fr not_active Ceased
- 2005-05-24 AU AU2005242054A patent/AU2005242054B2/en not_active Ceased
- 2005-05-24 BR BRPI0506556-9A patent/BRPI0506556A/pt not_active IP Right Cessation
- 2005-05-24 CN CN2005800071699A patent/CN1954391B/zh not_active Expired - Fee Related
- 2005-05-24 JP JP2007542959A patent/JP2008522362A/ja not_active Withdrawn
- 2005-05-24 CA CA002538368A patent/CA2538368A1/fr not_active Abandoned
- 2005-05-24 WO PCT/RU2005/000284 patent/WO2005109970A1/fr active Application Filing
-
2012
- 2012-09-14 JP JP2012202531A patent/JP2013016507A/ja not_active Withdrawn
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2014
- 2014-12-25 JP JP2014263119A patent/JP2015092495A/ja active Pending
Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4292125A (en) * | 1978-08-21 | 1981-09-29 | Massachusetts Institute Of Technology | System and method for generating steady state confining current for a toroidal plasma fusion reactor |
| SU1216805A1 (ru) * | 1984-03-15 | 1986-03-07 | Предприятие П/Я В-8851 | Способ создани стационарного тока в плазме |
| RU2067360C1 (ru) * | 1994-01-25 | 1996-09-27 | Михаил Агеевич Поломарчук | Способ получения высокотемпературной плазмы |
| RU2096934C1 (ru) * | 1995-11-29 | 1997-11-20 | Милья Аркадьевич Маргулис | Способ получения высокотемпературной плазмы и осуществления термоядерных реакций |
Non-Patent Citations (2)
| Title |
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| LUKYANOV S. JU.: "Nauka.", 1975, pages 115 - 116 * |
| See also references of EP1673966A4 * |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2013016507A (ja) * | 2004-11-30 | 2013-01-24 | Zakrytoe Aktsionernoe Obschestvo Rustermosintez | 高密度高温プラズマの安定状態を形成する方法 |
| WO2008063254A2 (fr) * | 2006-08-18 | 2008-05-29 | Unified Gravity Corporation | Dispositif de fusion hydrogène-lithium, procédé et applications |
| WO2008063254A3 (fr) * | 2006-08-18 | 2008-12-31 | Unified Gravity Corp | Dispositif de fusion hydrogène-lithium, procédé et applications |
Also Published As
| Publication number | Publication date |
|---|---|
| RU2273968C1 (ru) | 2006-04-10 |
| BRPI0506556A (pt) | 2007-04-17 |
| CA2538368A1 (fr) | 2005-11-17 |
| AU2005242054B2 (en) | 2008-11-27 |
| CN1954391A (zh) | 2007-04-25 |
| JP2013016507A (ja) | 2013-01-24 |
| KR20070050003A (ko) | 2007-05-14 |
| NZ548650A (en) | 2012-09-28 |
| JP2008522362A (ja) | 2008-06-26 |
| JP2015092495A (ja) | 2015-05-14 |
| EP1673966A4 (fr) | 2009-08-12 |
| EP1673966A1 (fr) | 2006-06-28 |
| KR100877367B1 (ko) | 2009-01-09 |
| AU2005242054A1 (en) | 2005-11-17 |
| CN1954391B (zh) | 2012-07-04 |
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